Abstract
The $b$-axis dielectric anomaly at the commensurate-incommensurate phase-transition temperature in BaMn${\mathrm{F}}_{4}$ has been calculated. Its shape and magnitude agree with the data of Samara and Richards. The $a$-axis anomaly below ${T}_{N}$ is also explained; its shape and magnitude are due to the canting of Mn spins. It is a first-order effect and \ensuremath{\sim} ${10}^{5}$ larger than in Rado's second-order theory for ${\mathrm{Cr}}_{2}$${\mathrm{O}}_{3}$.
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Publication Info
- Year
- 1977
- Type
- article
- Volume
- 16
- Issue
- 5
- Pages
- 2329-2331
- Citations
- 71
- Access
- Closed
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- DOI
- 10.1103/physrevb.16.2329